Search Results - "Deile, M."

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    3D Active Edge Silicon Detector Tests With 120 GeV Muons by Da Via, C., Deile, M., Hasi, J., Kenney, C., Kok, A., Parker, S., Watts, S., Anelli, G., Avati, V., Bassetti, V., Boccone, V., Bozzo, M., Eggert, K., Ferro, F., Inyakin, A., Kaplon, J., Bahilo, J.L., Morelli, A., Niewiadomski, H., Noschis, E., Oljemark, F., Oriunno, M., Osterberg, K., Ruggiero, G., Snoeys, W., Tapprogge, S.

    Published in IEEE transactions on nuclear science (01-04-2009)
    “…3D detectors with electrodes penetrating through the silicon wafer and covering the edges were tested in the SPS beam line X5 at CERN in autumn 2003. Detector…”
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    Journal Article
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    Performance of the ATLAS precision muon chambers under LHC operating conditions by Deile, M., Dietl, H., Dubbert, J., Horvat, S., Kortner, O., Kroha, H., Manz, A., Mohrdieck, S., Rauscher, F., Richter, R., Staude, A.

    “…For the muon spectrometer of the ATLAS detector at the Large Hadron Collider (LHC), large drift chambers consisting of 6–8 layers of pressurized drift tubes…”
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    Construction and test of MDT chambers for the ATLAS muon spectrometer by Bauer, F., Bratzler, U., Dietl, H., Kroha, H., Lagouri, Th, Manz, A., Ostapchuk, A., Richter, R., Schael, S., Chouridou, S., Deile, M., Kortner, O., Staude, A., Ströhmer, R., Trefzger, T.

    “…The Monitored Drift Tube (MDT) chambers for the muon spectrometer of the ATLAS detector at the Large Hadron Collider (LHC) consist of 3–4 layers of pressurized…”
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    First measurement of elastic, inelastic and total cross-section at s=13 TeV by TOTEM and overview of cross-section data at LHC energies: TOTEM Collaboration by Antchev, G., Aspell, P., Atanassov, I., Avati, V., Baechler, J., Barrera, C. Baldenegro, Berardi, V., Berretti, M., Bossini, E., Bottigli, U., Bozzo, M., Burkhardt, H., Cafagna, F. S., Catanesi, M. G., Csanád, M., Csörgő, T., Deile, M., De Leonardis, F., D’Orazio, A., Doubek, M., Druzhkin, D., Eggert, K., Eremin, V., Ferro, F., Fiergolski, A., Garcia, F., Georgiev, V., Giani, S., Grzanka, L., Hammerbauer, J., Heino, J., Helander, P., Isidori, T., Ivanchenko, V., Janda, M., Karev, A., Kašpar, J., Kopal, J., Kundrát, V., Lami, S., Latino, G., Lauhakangas, R., Linhart, R., Lindsey, C., Lokajíček, M. V., Losurdo, L., Vetere, M. Lo, Rodríguez, F. Lucas, Macrí, M., Malawski, M., Minafra, N., Minutoli, S., Naaranoja, T., Nemes, F., Niewiadomski, H., Novák, T., Oliveri, E., Oljemark, F., Oriunno, M., Österberg, K., Palazzi, P., Passaro, V., Peroutka, Z., Procházka, J., Quinto, M., Radermacher, E., Radicioni, E., Ravotti, F., Robutti, E., Royon, C., Ruggiero, G., Saarikko, H., Scribano, A., Siroky, J., Smajek, J., Snoeys, W., Stefanovitch, R., Sziklai, J., Taylor, C., Tcherniaev, E., Turini, N., Vacek, V., Welti, J., Williams, J., Wyszkowski, P., Zich, J., Zielinski, K.

    “…The TOTEM collaboration has measured the proton–proton total cross section at s = 13 TeV with a luminosity-independent method. Using dedicated β ∗ = 90 m beam…”
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    First determination of the ρ parameter at s=13 TeV: probing the existence of a colourless C-odd three-gluon compound state: TOTEM Collaboration by Antchev, G., Aspell, P., Atanassov, I., Avati, V., Baechler, J., Barrera, C. Baldenegro, Berardi, V., Berretti, M., Bossini, E., Bottigli, U., Bozzo, M., Bruce, R., Burkhardt, H., Cafagna, F. S., Catanesi, M. G., Csanád, M., Csörgő, T., Deile, M., De Leonardis, F., D’Orazio, A., Doubek, M., Druzhkin, D., Eggert, K., Eremin, V., Ferro, F., Fiergolski, A., Garcia, F., Morales, H. Garcia, Georgiev, V., Giani, S., Grzanka, L., Hammerbauer, J., Heino, J., Helander, P., Isidori, T., Ivanchenko, V., Janda, M., Karev, A., Kašpar, J., Kopal, J., Kundrát, V., Lami, S., Latino, G., Lauhakangas, R., Linhart, R., Lindsey, C., Lokajíček, M. V., Losurdo, L., Lo Vetere, M., Rodríguez, F. Lucas, Macrí, M., Malawski, M., Mereghetti, A., Minafra, N., Minutoli, S., Mirarchi, D., Naaranoja, T., Nemes, F., Niewiadomski, H., Novák, T., Oliveri, E., Oljemark, F., Oriunno, M., Österberg, K., Palazzi, P., Passaro, V., Peroutka, Z., Procházka, J., Quinto, M., Radermacher, E., Radicioni, E., Ravotti, F., Redaelli, S., Robutti, E., Royon, C., Ruggiero, G., Saarikko, H., Salvachua, B., Scribano, A., Siroky, J., Smajek, J., Snoeys, W., Stefanovitch, R., Sziklai, J., Taylor, C., Tcherniaev, E., Turini, N., Vacek, V., Valentino, G., Welti, J., Wenninger, J., Williams, J., Wyszkowski, P., Zich, J., Zielinski, K.

    “…The TOTEM experiment at the LHC has performed the first measurement at s = 13 TeV of the ρ parameter, the real to imaginary ratio of the nuclear elastic…”
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    Measurement of elastic pp scattering at s=8 TeV in the Coulomb–nuclear interference region: determination of the ρ-parameter and the total cross-section by Antchev, G., Aspell, P., Atanassov, I., Avati, V., Baechler, J., Berardi, V., Berretti, M., Bossini, E., Bottigli, U., Bozzo, M., Broulím, P., Burkhardt, H., Buzzo, A., Cafagna, F. S., Campanella, C. E., Catanesi, M. G., Csanád, M., Csörgő, T., Deile, M., De Leonardis, F., D’Orazio, A., Doubek, M., Eggert, K., Eremin, V., Ferro, F., Fiergolski, A., Garcia, F., Georgiev, V., Giani, S., Grzanka, L., Guaragnella, C., Hammerbauer, J., Heino, J., Karev, A., Kašpar, J., Kopal, J., Kundrát, V., Lami, S., Latino, G., Lauhakangas, R., Linhart, R., Lippmaa, E., Lippmaa, J., Lokajíček, M. V., Losurdo, L., Lo Vetere, M., Lucas Rodríguez, F., Macrí, M., Mercadante, A., Minafra, N., Minutoli, S., Naaranoja, T., Nemes, F., Niewiadomski, H., Oliveri, E., Oljemark, F., Orava, R., Oriunno, M., Österberg, K., Palazzi, P., Paločko, L., Passaro, V., Peroutka, Z., Petruzzelli, V., Politi, T., Procházka, J., Prudenzano, F., Quinto, M., Radermacher, E., Radicioni, E., Ravotti, F., Redaelli, S., Robutti, E., Ropelewski, L., Ruggiero, G., Saarikko, H., Salvachua, B., Scribano, A., Smajek, J., Snoeys, W., Sziklai, J., Taylor, C., Turini, N., Vacek, V., Valentino, G., Welti, J., Wenninger, J., Wyszkowski, P., Zielinski, K.

    “…The TOTEM experiment at the CERN LHC has measured elastic proton–proton scattering at the centre-of-mass energy s = 8 TeV and four-momentum transfers squared,…”
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    Rate effects in high-resolution drift chambers by Aleksa, M., Deile, M., Dubbert, J., Fabjan, C.W., Gruhn, C., Hessey, N.P., Riegler, W., Sammer, T.

    “…The impact of high counting rates on the spatial resolution of cylindrical drift tubes is investigated in detail and the results are compared with simulations…”
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    Resolution limits of drift tubes by Riegler, W., Aleksa, M., Deile, M., Dubbert, J., Fabjan, C.W., Gruhn, C., Hessey, N.P., Sammer, T.

    “…Measurements of the drift-tube response to charged particle tracks are compared with a complete simulation. The measured resolution of typically 80 μm agrees…”
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    Construction and test of the precision drift chambers for the ATLAS muon spectrometer by Bauer, F., Blum, W., Bratzler, U., Dietl, H., Kotov, S., Kroha, H., Lagouri, T., Manz, A., Ostapchuk, A., Richter, R., Schael, S., Chouridou, S., Deile, M., Kornter, O., Staude, A., Strohmer, R., Trefzger, T.

    Published in IEEE transactions on nuclear science (01-06-2001)
    “…The monitored drift tube (MDT) chambers for the muon spectrometer of the ATLAS detector at the Large Hadron Collider (LHC) consist of three or four layers of…”
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    Journal Article